The energy difference (\(\Delta E\)) for a hydrogen atom transition, absorbed or emitted light's wavelength (\(\lambda\)), is defined by \(\Delta E = \frac{R_H}{n_1^2} - \frac{R_H}{n_2^2}\), where \(R_H\) is the Rydberg constant and \(n_1, n_2\) are the principal quantum numbers of the initial and final orbits. Energy and wavelength are inversely proportional: \(E = \frac{hc}{\lambda}\), with \(h\) as Planck's constant and \(c\) as the speed of light. Consequently, wavelength ratios are the inverse of energy ratios.
Calculations for energy differences of two transitions:
1. For \(n = 2 \rightarrow n = 3\): \[\Delta E_1 = \frac{R_H}{2^2} - \frac{R_H}{3^2} = R_H \left( \frac{1}{4} - \frac{1}{9} \right) = R_H \times \frac{5}{36}\]
2. For \(n = 4 \rightarrow n = 6\): \[\Delta E_2 = \frac{R_H}{4^2} - \frac{R_H}{6^2} = R_H \left( \frac{1}{16} - \frac{1}{36} \right) = R_H \times \frac{5}{144}\]
The ratio of wavelengths (\(\lambda_1 / \lambda_2\)) equals the inverse ratio of energy differences:
\[\frac{\lambda_1}{\lambda_2} = \frac{\Delta E_2}{\Delta E_1} = \frac{\frac{5}{144}}{\frac{5}{36}} = \frac{36}{144} = \frac{1}{4}\]
Thus, the ratio of wavelengths is 1 : 4.
Therefore, the correct answer is (3) 1 : 4.